Effectiveness factor at isothermal conditions
For an irreversible first order reaction A → B
, at isothermal condition the rate at surface condition can be written as
. Then the actual global rate at outer surface condition,
.
For a spherical catalyst pellet of radius ‘Rs', mass balance over a spherical shell volume of thickness
at steady state will be:
(Rate of diffusion of reactant into element) – (Rate of diffusion of reactant out of element) = Rate of disappearance of reactant within element due to reaction

Rate of reaction per unit mass of catalyst = ![]()
Rate of reaction per unit volume of catalyst =
.
Where
is the density of pellet.
Then the mass balance equation over the element of thickness
can be written as
![]()
If limit is taken as
and assuming that effective diffusivity is independent of concentration of reactant the above equation can be written as
![]() |
(7) |
Boundary conditions:
| At the center of the pellet, | (8) |
| At outer surface | (9) |
Solving the differential equation (7) with boundary conditions (8) and (9) following relation is obtained
| (10) |
Where
is a dimensionless group defined as
![]() |
|

